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Page 395
... mass M at rest into two particles of mass m1 and m2 M → m1 + m2 ( 12.14 ) can occur if the initial mass is greater than the sum of the final masses . We define the mass excess AM : AM = M - m1 - m2 ( 12.15 ) The sum of the kinetic ...
... mass M at rest into two particles of mass m1 and m2 M → m1 + m2 ( 12.14 ) can occur if the initial mass is greater than the sum of the final masses . We define the mass excess AM : AM = M - m1 - m2 ( 12.15 ) The sum of the kinetic ...
Page 400
... mass , the mass difference is AM = m „ o 135.0 Mev , while the target mass is m2 = m , = 938.5 Mev . Then the threshold energy is Tth = 135.0 [ 1 1 + 135.0 2 ( 938.5 ) = 135.0 ( 1.072 ) = 144.7 Mev As another example consider the ...
... mass , the mass difference is AM = m „ o 135.0 Mev , while the target mass is m2 = m , = 938.5 Mev . Then the threshold energy is Tth = 135.0 [ 1 1 + 135.0 2 ( 938.5 ) = 135.0 ( 1.072 ) = 144.7 Mev As another example consider the ...
Page 589
... mass . 17.4 Difficulties with the Abraham - Lorentz Model Although the Abraham - Lorentz approach is a significant step towards a fundamental description of a charged particle , it is deficient in several respects . 1. One obvious ...
... mass . 17.4 Difficulties with the Abraham - Lorentz Model Although the Abraham - Lorentz approach is a significant step towards a fundamental description of a charged particle , it is deficient in several respects . 1. One obvious ...
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation frequency given Green's function impact parameter incident particle integral Kirchhoff Lagrangian Laplace's equation Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain oscillations P₁ parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ